TY - JOUR
T1 - Thermoelectric properties of Co-, Ir-, and Os-doped FeSi alloys
T2 - Evidence for strong electron-phonon coupling
AU - Sales, Brian C.
AU - Delaire, Olivier
AU - McGuire, Michael A.
AU - May, Andrew F.
PY - 2011/3/28
Y1 - 2011/3/28
N2 - The effects of various transition-metal dopants on the electrical and thermal transport properties of Fe1-xMxSi alloys (M = Co, Ir, Os) are reported. The maximum thermoelectric figure of merit ZT max is improved from 0.007 at 60 K for pure FeSi to ZT = 0.08 at 100 K for 4% Ir doping. A comparison of the thermal conductivity data among Os-, Ir-, and Co-doped alloys indicates strong electron-phonon coupling in this compound. Because of this interaction, the common approximation of dividing the total thermal conductivity into independent electronic and lattice components (κtotal = κelectronic + κ lattice) fails for these alloys. The effects of grain size on thermoelectric properties of Fe0.96Ir0.04Si alloys are also reported. The thermal conductivity can be lowered by ∼50% with little or no effect on the electrical resistivity or Seebeck coefficient. This results in ZTmax = 0.125 at 100 K, still approximately a factor of 5 too low for solid-state refrigeration applications.
AB - The effects of various transition-metal dopants on the electrical and thermal transport properties of Fe1-xMxSi alloys (M = Co, Ir, Os) are reported. The maximum thermoelectric figure of merit ZT max is improved from 0.007 at 60 K for pure FeSi to ZT = 0.08 at 100 K for 4% Ir doping. A comparison of the thermal conductivity data among Os-, Ir-, and Co-doped alloys indicates strong electron-phonon coupling in this compound. Because of this interaction, the common approximation of dividing the total thermal conductivity into independent electronic and lattice components (κtotal = κelectronic + κ lattice) fails for these alloys. The effects of grain size on thermoelectric properties of Fe0.96Ir0.04Si alloys are also reported. The thermal conductivity can be lowered by ∼50% with little or no effect on the electrical resistivity or Seebeck coefficient. This results in ZTmax = 0.125 at 100 K, still approximately a factor of 5 too low for solid-state refrigeration applications.
UR - http://www.scopus.com/inward/record.url?scp=79961058531&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.83.125209
DO - 10.1103/PhysRevB.83.125209
M3 - Article
AN - SCOPUS:79961058531
SN - 1098-0121
VL - 83
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 12
M1 - 125209
ER -